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Trigonometry

Radian Measure

Definition

The radian is the standard unit of angular measure. An angle θ\theta in radians is defined as the Ratio of the arc length ss subtended by the angle to the radius rr:

θ={s}{r}\theta = \frac\{s\}\{r\}

One radian is the angle subtended at the centre of a circle by an arc equal in length to the radius. Since the circumference of a circle is 2πr2\pi r A full revolution is 2π2\pi radians.

Conversion Between Degrees and Radians

π{rad}=180{∘}\pi \mathrm\{ rad\} = 180^\{\circ\}

To convert from degrees to radians:

θ{{rad}}=θ{{deg}}×{π}{180}\theta_\{\mathrm\{rad\}\} = \theta_\{\mathrm\{deg\}\} \times \frac\{\pi\}\{180\}

To convert from radians to degrees:

θ{{deg}}=θ{{rad}}×{180}{π}\theta_\{\mathrm\{deg\}\} = \theta_\{\mathrm\{rad\}\} \times \frac\{180\}\{\pi\}

Arc Length

For a circle of radius rr with a central angle θ\theta (in radians):

S=rθS = r\theta

Sector Area

The area of a sector with central angle θ\theta (in radians) and radius rr:

A={1}{2}r2θA = \frac\{1\}\{2\}r^2\theta

Worked Example: Arc Length and Sector Area

Problem: A sector has radius 55 cm and central angle 3π4\frac{3\pi}{4} radians. Find the arc Length and the area of the sector.

Solution:

Arc length:

S=rθ=5×{3π}{4}={15π}{4}≈11.78{cm}S = r\theta = 5 \times \frac\{3\pi\}\{4\} = \frac\{15\pi\}\{4\} \approx 11.78 \mathrm\{ cm\}

Sector area:

A={1}{2}r2θ={1}{2}(25)({3π}{4})={75π}{8}≈29.45{cm}2A = \frac\{1\}\{2\}r^2\theta = \frac\{1\}\{2\}(25)\left(\frac\{3\pi\}\{4\}\right) = \frac\{75\pi\}\{8\} \approx 29.45 \mathrm\{ cm\}^2

Trigonometric Functions

Right-Angle Definitions

sin⁡θ=oppositehypotenuse,cos⁡θ=adjacenthypotenuse,tan⁡θ=oppositeadjacent=sin⁡θcos⁡θ\sin \theta = \frac{\mathrm{opposite}}{\mathrm{hypotenuse}}, \quad \cos \theta = \frac{\mathrm{adjacent}}{\mathrm{hypotenuse}}, \quad \tan \theta = \frac{\mathrm{opposite}}{\mathrm{adjacent}} = \frac{\sin \theta}{\cos \theta}

Reciprocal Trigonometric Functions

csc⁡θ={1}{sin⁡θ},sec⁡θ={1}{cos⁡θ},cot⁡θ={1}{tan⁡θ}={cos⁡θ}{sin⁡θ}\csc\theta = \frac\{1\}\{\sin\theta\}, \quad \sec\theta = \frac\{1\}\{\cos\theta\}, \quad \cot\theta = \frac\{1\}\{\tan\theta\} = \frac\{\cos\theta\}\{\sin\theta\}

These are defined wherever the denominator is non-zero.

Graphs of Reciprocal Functions

FunctionDomainRangeAsymptotesxx-intercepts
y=csc⁡xy = \csc xx≠nπx \neq n\piy≤−1y \le -1 or y≥1y \ge 1x=nπx = n\pinone
y=sec⁡xy = \sec xx≠π2+nπx \neq \frac{\pi}{2} + n\piy≤−1y \le -1 or y≥1y \ge 1x=π2+nπx = \frac{\pi}{2} + n\pinone
y=cot⁡xy = \cot xx≠nπx \neq n\piall real yyx=nπx = n\pix=π2+nπx = \frac{\pi}{2} + n\pi

The Unit Circle

The unit circle is a circle of radius 11 centred at the origin. Any point on the unit circle has Coordinates (cos⁡θ,sin⁡θ)(\cos\theta, \sin\theta) Where θ\theta is the angle measured anticlockwise from the Positive xx-axis.

This definition extends trigonometric functions to all real numbers, not just acute angles. The Pythagorean identity follows directly from the fact that every point on the unit circle satisfies x2+y2=1x^2 + y^2 = 1.

Key Values

θ\theta00π6\frac{\pi}{6}π4\frac{\pi}{4}π3\frac{\pi}{3}π2\frac{\pi}{2}π\pi3π2\frac{3\pi}{2}2π2\pi
sin⁡θ\sin\theta0012\frac{1}{2}22\frac{\sqrt{2}}{2}32\frac{\sqrt{3}}{2}1100−1-100
cos⁡θ\cos\theta1132\frac{\sqrt{3}}{2}22\frac{\sqrt{2}}{2}12\frac{1}{2}00−1-10011
tan⁡θ\tan\theta0013\frac{1}{\sqrt{3}}113\sqrt{3}undefined00undefined00

All, Sine, Tan, Cos (ASTC)

The signs of trig functions in each quadrant:

  • All positive in the first quadrant (0<θ<π20 \lt \theta \lt \frac{\pi}{2})
  • Sine positive in the second quadrant (π2<θ<π\frac{\pi}{2} \lt \theta \lt \pi)
  • Tangent positive in the third quadrant (π<θ<3π2\pi \lt \theta \lt \frac{3\pi}{2})
  • Cosine positive in the fourth quadrant (3π2<θ<2π\frac{3\pi}{2} \lt \theta \lt 2\pi)

Graphs of Trigonometric Functions

y=sin⁡xy = \sin x

  • Domain: all real xx
  • Range: −1≤y≤1-1 \le y \le 1
  • Period: 2π2\pi
  • xx-intercepts at x=0,π,2π,…x = 0, \pi, 2\pi, \ldots

y=cos⁡xy = \cos x

  • Domain: all real xx
  • Range: −1≤y≤1-1 \le y \le 1
  • Period: 2π2\pi
  • yy-intercept at (0,1)(0, 1)

y=tan⁡xy = \tan x

  • Domain: all real xx except x=π2+nπx = \frac{\pi}{2} + n\pi
  • Range: all real yy
  • Period: π\pi
  • Vertical asymptotes at x=π2+nπx = \frac{\pi}{2} + n\pi

Transformations

For y=asin⁡(bx+c)+dy = a\sin(bx + c) + d:

  • ∣a∣|a| = amplitude
  • 2π∣b∣\frac{2\pi}{|b|} = period
  • cc = horizontal phase shift (shift left by cb\frac{c}{b})
  • dd = vertical shift

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Use the sliders to see how changing aa, bb, cc And dd in y=asin⁡(bx+c)+dy = a\sin(bx + c) + d affects the Graph.

Trigonometric Identities

Pythagorean Identities

\begin`\{aligned}` \sin^2\theta + \cos^2\theta &= 1\\ 1 + \tan^2\theta &= \sec^2\theta\\ 1 + \cot^2\theta &= \csc^2\theta \end`\{aligned}`

Proof of sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1

By the unit circle definition, a point on the unit circle at angle θ\theta has coordinates (cos⁡θ,sin⁡θ)(\cos\theta, \sin\theta). Since every point on the unit circle satisfies x2+y2=1x^2 + y^2 = 1 We Substitute:

cos⁡2θ+sin⁡2θ=1\cos^2\theta + \sin^2\theta = 1

This completes the …/1-number-and-algebra/3_proof-and-logic.

Proof of 1+tan⁡2θ=sec⁡2θ1 + \tan^2\theta = \sec^2\theta

Starting from sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1 Divide both sides by cos⁡2θ\cos^2\theta:

{sin⁡2θ}{cos⁡2θ}+{cos⁡2θ}{cos⁡2θ}={1}{cos⁡2θ}\frac\{\sin^2\theta\}\{\cos^2\theta\} + \frac\{\cos^2\theta\}\{\cos^2\theta\} = \frac\{1\}\{\cos^2\theta\} tan⁡2θ+1=sec⁡2θ\tan^2\theta + 1 = \sec^2\theta

Proof of 1+cot⁡2θ=csc⁡2θ1 + \cot^2\theta = \csc^2\theta

Starting from sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1 Divide both sides by sin⁡2θ\sin^2\theta:

{sin⁡2θ}{sin⁡2θ}+{cos⁡2θ}{sin⁡2θ}={1}{sin⁡2θ}\frac\{\sin^2\theta\}\{\sin^2\theta\} + \frac\{\cos^2\theta\}\{\sin^2\theta\} = \frac\{1\}\{\sin^2\theta\} 1+cot⁡2θ=csc⁡2θ1 + \cot^2\theta = \csc^2\theta

Compound Angle Identities

\begin`\{aligned}` \sin(A \pm B) &= \sin A \cos B \pm \cos A \sin B\\ \cos(A \pm B) &= \cos A \cos B \mp \sin A \sin B\\ \tan(A \pm B) &= \frac\{\tan A \pm \tan B\}\{1 \mp \tan A \tan B\} \end`\{aligned}`

Proof of Compound Angle Formulas (Rotation Matrix)

Consider rotating the point (1,0)(1, 0) by angle A+BA + B anticlockwise. The resulting coordinates are (cos⁡(A+B),sin⁡(A+B))(\cos(A + B), \sin(A + B)).

Equivalently, we can first rotate by BB Then by AA. The rotation matrix for angle α\alpha is:

R(\alpha) = \begin`\{pmatrix}` \cos\alpha & -\sin\alpha \\ \sin\alpha & \cos\alpha \end`\{pmatrix}`

The composite rotation R(A)R(B)R(A)R(B) applied to (1,0)(1, 0):

\begin`\{pmatrix}` \cos A & -\sin A \\ \sin A & \cos A \end`\{pmatrix}` \begin`\{pmatrix}` \cos B & -\sin B \\ \sin B & \cos B \end`\{pmatrix}` \begin`\{pmatrix}` 1 \\ 0 \end`\{pmatrix}`

First multiply the matrices:

R(A)R(B) = \begin`\{pmatrix}` \cos A \cos B - \sin A \sin B & -\cos A \sin B - \sin A \cos B \\ \sin A \cos B + \cos A \sin B & -\sin A \sin B + \cos A \cos B \end`\{pmatrix}`

Applying to (1,0)(1, 0) gives the top-left and bottom-left entries:

cos⁡(A+B)=cos⁡Acos⁡B−sin⁡Asin⁡B,sin⁡(A+B)=sin⁡Acos⁡B+cos⁡Asin⁡B\cos(A + B) = \cos A \cos B - \sin A \sin B, \quad \sin(A + B) = \sin A \cos B + \cos A \sin B

The formulas for A−BA - B follow by substituting −B-B and using sin⁡(−B)=−sin⁡B\sin(-B) = -\sin B cos⁡(−B)=cos⁡B\cos(-B) = \cos B.

Double Angle Identities

Setting A=B=θA = B = \theta in the compound angle formulas:

\begin`\{aligned}` \sin 2\theta &= 2\sin\theta \cos\theta\\[4pt] \cos 2\theta &= \cos^2\theta - \sin^2\theta\\ \tan 2\theta &= \frac\{2\tan\theta\}\{1 - \tan^2\theta\} \end`\{aligned}`

Three Forms of cos⁡2θ\cos 2\theta

Starting from cos⁡2θ=cos⁡2θ−sin⁡2θ\cos 2\theta = \cos^2\theta - \sin^2\theta:

  • Form 1: cos⁡2θ=cos⁡2θ−sin⁡2θ\cos 2\theta = \cos^2\theta - \sin^2\theta
  • Form 2: Replace sin⁡2θ=1−cos⁡2θ\sin^2\theta = 1 - \cos^2\theta: cos⁡2θ=2cos⁡2θ−1\cos 2\theta = 2\cos^2\theta - 1
  • Form 3: Replace cos⁡2θ=1−sin⁡2θ\cos^2\theta = 1 - \sin^2\theta: cos⁡2θ=1−2sin⁡2θ\cos 2\theta = 1 - 2\sin^2\theta

Triple Angle Identities

sin⁡3θ=3sin⁡θ−4sin⁡3θ\sin 3\theta = 3\sin\theta - 4\sin^3\theta

Derivation: Using sin⁡(2θ+θ)\sin(2\theta + \theta):

sin⁡3θ=sin⁡2θcos⁡θ+cos⁡2θsin⁡θ=2sin⁡θcos⁡2θ+(1−2sin⁡2θ)sin⁡θ=2sin⁡θ(1−sin⁡2θ)+sin⁡θ−2sin⁡3θ=3sin⁡θ−4sin⁡3θ\sin 3\theta = \sin 2\theta \cos\theta + \cos 2\theta \sin\theta = 2\sin\theta\cos^2\theta + (1 - 2\sin^2\theta)\sin\theta = 2\sin\theta(1 - \sin^2\theta) + \sin\theta - 2\sin^3\theta = 3\sin\theta - 4\sin^3\theta

Inverse Trigonometric Functions

FunctionMeaningDomainRange
arcsin⁡x\arcsin x”the angle whose sine is xx"−1≤x≤1-1 \le x \le 1−π2≤arcsin⁡x≤π2-\frac{\pi}{2} \le \arcsin x \le \frac{\pi}{2}
arccos⁡x\arccos x"the angle whose cosine is xx"−1≤x≤1-1 \le x \le 10≤arccos⁡x≤π0 \le \arccos x \le \pi
arctan⁡x\arctan x"the angle whose tangent is xx“all real xx−π2<arctan⁡x<π2-\frac{\pi}{2} \lt \arctan x \lt \frac{\pi}{2}

Properties

arcsin⁡(−x)=−arcsin⁡(x),arctan⁡(−x)=−arctan⁡(x),arccos⁡(−x)=π−arccos⁡(x)\arcsin(-x) = -\arcsin(x), \quad \arctan(-x) = -\arctan(x), \quad \arccos(-x) = \pi - \arccos(x)

Composition Identities

For xx in the appropriate domain:

\begin`\{aligned}` \sin(\arcsin x) &= x, \quad \mathrm\{for \} -1 \le x \le 1\\ \cos(\arccos x) &= x, \quad \mathrm\{for \} -1 \le x \le 1\\ \tan(\arctan x) &= x, \quad \mathrm\{for all real \} x \end`\{aligned}`

The reverse compositions are only true on restricted domains:

\begin`\{aligned}` \arcsin(\sin x) &= x, \quad \mathrm\{for \} -\frac\{\pi\}\{2\} \le x \le \frac\{\pi\}\{2\}\\ \arccos(\cos x) &= x, \quad \mathrm\{for \} 0 \le x \le \pi\\ \arctan(\tan x) &= x, \quad \mathrm\{for \} -\frac\{\pi\}\{2\} \lt x \lt \frac\{\pi\}\{2\} \end`\{aligned}`

Worked Example: Inverse Trig Evaluation

Problem: Evaluate sin⁡(arccos⁡13)\sin\left(\arccos\frac{1}{3}\right) without a calculator.

Solution:

Let θ=arccos⁡13\theta = \arccos\frac{1}{3} So cos⁡θ=13\cos\theta = \frac{1}{3} with θ∈[0,π]\theta \in [0, \pi]. Since cos⁡θ>0\cos\theta \gt 0 We have θ\theta in the first quadrant, so sin⁡θ≥0\sin\theta \ge 0:

sin⁡θ={1−{1}{9}}={2{2}}{3}\sin\theta = \sqrt\{1 - \frac\{1\}\{9\}\} = \frac\{2\sqrt\{2\}\}\{3\}

Sine and Cosine Rules

Sine Rule

{a}{sin⁡A}={b}{sin⁡B}={c}{sin⁡C}\frac\{a\}\{\sin A\} = \frac\{b\}\{\sin B\} = \frac\{c\}\{\sin C\}

Used when you know:

  • Two angles and one side (AAS), or
  • Two sides and a non-included angle (SSA — see ambiguous case below)

Cosine Rule

C2=a2+b2−2abcos⁡CC^2 = a^2 + b^2 - 2ab\cos C

Or equivalently:

cos⁡C={a2+b2−c2}{2ab}\cos C = \frac\{a^2 + b^2 - c^2\}\{2ab\}

Used when you know:

  • Two sides and the included angle (SAS), or
  • All three sides (SSS)

Area of a Triangle

{Area}={1}{2}absin⁡C\mathrm\{Area\} = \frac\{1\}\{2\}ab\sin C

Worked Example: Sine Rule

Problem: In triangle ABC$$a = 8 cm, A = 45^\circ$$B = 30^\circ. Find bb.

Solution:

B=8sin⁡30∘sin⁡45∘=4{22}=42≈5.66cmB = \frac{8\sin 30^{\circ}}{\sin 45^{\circ}} = \frac{4}\{\frac{\sqrt{2}}{2}\} = 4\sqrt{2} \approx 5.66 \mathrm{ cm}

Worked Example: Cosine Rule

Problem: Find the angle CC in a triangle with sides a = 5$$b = 7$$c = 8.

Solution:

cos⁡C={52+72−82}{2×5×7}={25+49−64}{70}={10}{70}={1}{7}\cos C = \frac\{5^2 + 7^2 - 8^2\}\{2 \times 5 \times 7\} = \frac\{25 + 49 - 64\}\{70\} = \frac\{10\}\{70\} = \frac\{1\}\{7\} C=arccos⁡({1}{7})≈81.8{∘}C = \arccos\left(\frac\{1\}\{7\}\right) \approx 81.8^\{\circ\}

Ambiguous Case of the Sine Rule

When using the sine rule with SSA (two sides and a non-included angle), there may be two possible Triangles, one triangle, or no triangle.

Condition for Ambiguity

Given sides aa and bb and angle AA (where aa is opposite AA):

  • No triangle if a<bsin⁡Aa \lt b\sin A
  • One right-angled triangle if a=bsin⁡Aa = b\sin A
  • Two triangles if bsin⁡A<a<bb\sin A \lt a \lt b and A<90∘A \lt 90^\circ
  • One triangle if a≥ba \ge b or A≥90∘A \ge 90^\circ

Why Two Triangles?

When sin⁡B=k\sin B = k where 0<k<10 \lt k \lt 1 There are two possible values for BB:

B1=arcsin⁡(k){and}B2=180{∘}−arcsin⁡(k)B_1 = \arcsin(k) \quad \mathrm\{and\} \quad B_2 = 180^\{\circ\} - \arcsin(k)

Both may be valid since B1+B2=180∘B_1 + B_2 = 180^\circ (so if A+B1<180∘A + B_1 \lt 180^\circ Check whether A+B2<180∘A + B_2 \lt 180^\circ as well).

Worked Example: Ambiguous Case

Problem: In triangle ABC$$a = 7$$b = 10$$A = 40^\circ. Find all possible triangles.

Solution:

Using the sine rule:

{sin⁡B}{10}={sin⁡40{∘}}{7}  ⟹  sin⁡B={10sin⁡40{∘}}{7}≈0.919\frac\{\sin B\}\{10\} = \frac\{\sin 40^\{\circ\}\}\{7\} \implies \sin B = \frac\{10\sin 40^\{\circ\}\}\{7\} \approx 0.919

Since 0<0.919<10 \lt 0.919 \lt 1 There are two possible values for BB:

B1=arcsin⁡(0.919)≈66.8{∘},B2=180{∘}−66.8{∘}=113.2{∘}B_1 = \arcsin(0.919) \approx 66.8^\{\circ\}, \quad B_2 = 180^\{\circ\} - 66.8^\{\circ\} = 113.2^\{\circ\}

Check both: A+B1=106.8∘<180∘A + B_1 = 106.8^{\circ} \lt 180^\circ and A+B2=153.2∘<180∘A + B_2 = 153.2^{\circ} \lt 180^\circ. Both are valid.

Triangle 1: B = 66.8^\circ$$C = 73.2^\circ c1=7sin⁡73.2∘sin⁡40∘≈10.4c_1 = \frac{7\sin 73.2^{\circ}}{\sin 40^{\circ}} \approx 10.4

Triangle 2: B = 113.2^\circ$$C = 26.8^\circ c2=7sin⁡26.8∘sin⁡40∘≈4.89c_2 = \frac{7\sin 26.8^{\circ}}{\sin 40^{\circ}} \approx 4.89

Non-Right-Angled Triangle Problems

Strategy

  1. Draw and label a clear diagram.
  2. Identify which rule(s) to apply based on the given information.
  3. Use the sine rule for AAS or SSA, the cosine rule for SAS or SSS.
  4. For area problems, use 12absin⁡C\frac{1}{2}ab\sin C or split into right-angled triangles.
  5. For bearing problems, remember that bearings are measured clockwise from north.

Worked Example: Multi-Step Triangle Problem

Problem: In triangle ABC$$a = 12$$b = 8$$A = 65^\circ. Find the area of the triangle.

Solution:

Find angle BB using the sine rule:

{sin⁡B}{8}={sin⁡65{∘}}{12}  ⟹  sin⁡B={2sin⁡65{∘}}{3}≈0.604\frac\{\sin B\}\{8\} = \frac\{\sin 65^\{\circ\}\}\{12\} \implies \sin B = \frac\{2\sin 65^\{\circ\}\}\{3\} \approx 0.604

Since b<ab \lt a There is only one solution: B≈37.2∘B \approx 37.2^\circ So C=77.8∘C = 77.8^\circ.

{Area}={1}{2}(12)(8)sin⁡77.8{∘}≈47.0{squareunits}\mathrm\{Area\} = \frac\{1\}\{2\}(12)(8)\sin 77.8^\{\circ\} \approx 47.0 \mathrm\{ square units\}

Worked Example: Bearing Problem

Problem: A ship sails from port AA on a bearing of 050∘050^\circ for 1515 km to point BB Then On a bearing of 110∘110^\circ for 2020 km to point CC. Find the distance and bearing from CC back to AA.

Solution:

The angle at BB is the change in bearing: 110∘−050∘=60∘110^{\circ} - 050^{\circ} = 60^\circ. The interior angle at BB is 180∘−60∘=120∘180^{\circ} - 60^{\circ} = 120^\circ.

Using the cosine rule:

AC={152+202−2(15)(20)cos⁡120{∘}}={225+400+300}={925}=5{37}≈30.4{km}AC = \sqrt\{15^2 + 20^2 - 2(15)(20)\cos 120^\{\circ\}\} = \sqrt\{225 + 400 + 300\} = \sqrt\{925\} = 5\sqrt\{37\} \approx 30.4 \mathrm\{ km\}

To find the bearing, find angle CC:

{sin⁡C}{15}={sin⁡120{∘}}{5{37}}  ⟹  C≈25.3{∘}\frac\{\sin C\}\{15\} = \frac\{\sin 120^\{\circ\}\}\{5\sqrt\{37\}\} \implies C \approx 25.3^\{\circ\}

The bearing from CC to AA is 360∘−110∘−25.3∘≈225∘360^{\circ} - 110^{\circ} - 25.3^{\circ} \approx 225^\circ.

Solving Trigonometric Equations

General Solutions

\begin`\{aligned}` \sin\theta &= k \implies \theta = \arcsin(k) + 2n\pi \mathrm\{ or \} \theta = \pi - \arcsin(k) + 2n\pi\\ \cos\theta &= k \implies \theta = \arccos(k) + 2n\pi \mathrm\{ or \} \theta = -\arccos(k) + 2n\pi\\ \tan\theta &= k \implies \theta = \arctan(k) + n\pi \end`\{aligned}`

Where n∈Zn \in \mathbb{Z}.

Worked Example: Basic Trig Equation

Problem: Solve sin⁡2x=12\sin 2x = \frac{1}{2} for x∈[0,2π]x \in [0, 2\pi].

Solution:

Let u=2xu = 2x So u∈[0,4π]u \in [0, 4\pi].

sin⁡u={1}{2}  ⟹  u={π}{6},{5π}{6},2π+{π}{6},2π+{5π}{6}\sin u = \frac\{1\}\{2\} \implies u = \frac\{\pi\}\{6\}, \frac\{5\pi\}\{6\}, 2\pi + \frac\{\pi\}\{6\}, 2\pi + \frac\{5\pi\}\{6\} U={π}{6},{5π}{6},{13π}{6},{17π}{6}U = \frac\{\pi\}\{6\}, \frac\{5\pi\}\{6\}, \frac\{13\pi\}\{6\}, \frac\{17\pi\}\{6\} X={u}{2}={π}{12},{5π}{12},{13π}{12},{17π}{12}X = \frac\{u\}\{2\} = \frac\{\pi\}\{12\}, \frac\{5\pi\}\{12\}, \frac\{13\pi\}\{12\}, \frac\{17\pi\}\{12\}

Worked Example: Factoring

Problem: Solve 2cos⁡2x−cos⁡x−1=02\cos^2 x - \cos x - 1 = 0 for x∈[0,2π]x \in [0, 2\pi].

Solution:

Let u=cos⁡xu = \cos x:

2u2−u−1=0  ⟹  (2u+1)(u−1)=02u^2 - u - 1 = 0 \implies (2u + 1)(u - 1) = 0 U=−{1}{2}{or}u=1U = -\frac\{1\}\{2\} \mathrm\{ or \} u = 1
  • cos⁡x=−12  ⟹  x=2π3,4π3\cos x = -\frac{1}{2} \implies x = \frac{2\pi}{3}, \frac{4\pi}{3}
  • cos⁡x=1  ⟹  x=0\cos x = 1 \implies x = 0

So x=0,2π3,4π3x = 0, \frac{2\pi}{3}, \frac{4\pi}{3}.

Worked Example: Using Identities

Problem: Solve sin⁡2x=3cos⁡2x\sin^2 x = 3\cos^2 x for x∈[0,2π]x \in [0, 2\pi].

Solution:

Replace cos⁡2x\cos^2 x with 1−sin⁡2x1 - \sin^2 x:

sin⁡2x=3(1−sin⁡2x)  ⟹  sin⁡2x=3−3sin⁡2x  ⟹  4sin⁡2x=3\sin^2 x = 3(1 - \sin^2 x) \implies \sin^2 x = 3 - 3\sin^2 x \implies 4\sin^2 x = 3 sin⁡2x=34  ⟹  sin⁡x=±32\sin^2 x = \frac{3}{4} \implies \sin x = \pm\frac{\sqrt{3}}{2}

Since sin⁡x>0\sin x \gt 0 in quadrants I and II, and sin⁡x<0\sin x \lt 0 in quadrants III and IV:

X={π}{3},{2π}{3},{4π}{3},{5π}{3}X = \frac\{\pi\}\{3\}, \frac\{2\pi\}\{3\}, \frac\{4\pi\}\{3\}, \frac\{5\pi\}\{3\}

Worked Example: Equations Involving tan⁡\tan

Problem: Solve tan⁡2x=1\tan 2x = 1 for x∈[0,π]x \in [0, \pi].

Solution:

Since tan⁡\tan has period \pi$$\tan 2x = 1 gives 2x=π4+nπ2x = \frac{\pi}{4} + n\pi for n∈Zn \in \mathbb{Z}.

X={π}{8}+{nπ}{2}X = \frac\{\pi\}\{8\} + \frac\{n\pi\}\{2\}

For x∈[0,π]x \in [0, \pi]:

  • n=0n = 0: x=π8x = \frac{\pi}{8}
  • n=1n = 1: x=π8+π2=5π8x = \frac{\pi}{8} + \frac{\pi}{2} = \frac{5\pi}{8}
  • n=2n = 2: x=π8+π=9π8>πx = \frac{\pi}{8} + \pi = \frac{9\pi}{8} \gt \pi (outside range)

So x=π8,5π8x = \frac{\pi}{8}, \frac{5\pi}{8}.

Harmonic Form: Rsin⁡(x±α)R\sin(x \pm \alpha) and Rcos⁡(x±α)R\cos(x \pm \alpha)

Expressions of the form asin⁡x+bcos⁡xa\sin x + b\cos x can be written as a single trigonometric function:

Asin⁡x+bcos⁡x=Rsin⁡(x+α)A\sin x + b\cos x = R\sin(x + \alpha)

Where R=a2+b2R = \sqrt{a^2 + b^2} and tan⁡α=ba\tan\alpha = \frac{b}{a}.

This is useful for finding maximum/minimum values and for solving equations.

Worked Example: Harmonic Form

Problem: Express 3sin⁡x+4cos⁡x3\sin x + 4\cos x in the form Rsin⁡(x+α)R\sin(x + \alpha) And hence solve 3sin⁡x+4cos⁡x=53\sin x + 4\cos x = 5 for x∈[0,2π]x \in [0, 2\pi].

Solution:

R={32+42}=5R = \sqrt\{3^2 + 4^2\} = 5 tan⁡α={4}{3}  ⟹  α=arctan⁡{4}{3}≈0.927{rad}\tan\alpha = \frac\{4\}\{3\} \implies \alpha = \arctan\frac\{4\}\{3\} \approx 0.927 \mathrm\{ rad\}

So 3sin⁡x+4cos⁡x=5sin⁡(x+0.927)3\sin x + 4\cos x = 5\sin(x + 0.927).

Solving 5sin⁡(x+0.927)=55\sin(x + 0.927) = 5:

sin⁡(x+0.927)=1  ⟹  x+0.927={π}{2}+2nπ\sin(x + 0.927) = 1 \implies x + 0.927 = \frac\{\pi\}\{2\} + 2n\pi X={π}{2}−0.927+2nπ≈0.644+2nπX = \frac\{\pi\}\{2\} - 0.927 + 2n\pi \approx 0.644 + 2n\pi

For x∈[0,2π]x \in [0, 2\pi]: x≈0.644x \approx 0.644 rad (the next value 0.644+2π0.644 + 2\pi exceeds 2π2\pi).

3D Trigonometry

3D trigonometry involves applying trigonometric ratios in three-dimensional problems. The key is to Identify right-angled triangles within the 3D shape.

Strategy

  1. Draw a clear diagram of the 3D shape.
  2. Identify the relevant 2D triangles (often by drawing auxiliary lines).
  3. Label known sides and angles.
  4. Apply Pythagoras’ theorem, sine rule, cosine rule, or basic trig ratios.

Worked Example: 3D Problem

Problem: A pyramid has a square base of side 66 cm and vertical height 44 cm. Find the angle Between a sloping edge and the base.

Solution:

The distance from the centre of the base to a vertex is 622=32\frac{6\sqrt{2}}{2} = 3\sqrt{2} cm.

θ=arctan⁡({4}{3{2}})=arctan⁡({2{2}}{3})≈43.3{∘}\theta = \arctan\left(\frac\{4\}\{3\sqrt\{2\}\}\right) = \arctan\left(\frac\{2\sqrt\{2\}\}\{3\}\right) \approx 43.3^\{\circ\}

Trigonometric Proof Strategies

General Approach

In IB exams, trigonometric …/1-number-and-algebra/3_proof-and-logics ask you to show that one expression equals another. The Standard approach is:

  1. Start with one side — the more complex side (LHS).
  2. Apply known identities to transform it step by step toward the other side.
  3. Never assume what you are trying to prove — work forward from a known truth.

Useful Techniques

  • Factor: Look for common factors, e.g., sin⁡x+sin⁡xcos⁡x=sin⁡x(1+cos⁡x)\sin x + \sin x\cos x = \sin x(1 + \cos x).
  • Use sin⁡2+cos⁡2=1\sin^2 + \cos^2 = 1: Convert everything to sines or everything to cosines.
  • Convert to sin⁡\sin and cos⁡\cos: When \tan$$\sec$$\csc Or cot⁡\cot appear, express them in terms of sin⁡\sin and cos⁡\cos.
  • Look for compound angle structure: Recognise when an expression matches sin⁡(A±B)\sin(A \pm B) or cos⁡(A±B)\cos(A \pm B).
  • Common denominator: When fractions appear, combine them over a single denominator.

Worked Example: Proof by Multiplication

Problem: Prove that sin⁡x1+cos⁡x=1−cos⁡xsin⁡x\frac{\sin x}{1 + \cos x} = \frac{1 - \cos x}{\sin x}.

Proof:

Multiply numerator and denominator by 1−cos⁡x1 - \cos x:

{sin⁡x(1−cos⁡x)}{(1+cos⁡x)(1−cos⁡x)}={sin⁡x(1−cos⁡x)}{1−cos⁡2x}={sin⁡x(1−cos⁡x)}{sin⁡2x}={1−cos⁡x}{sin⁡x}={RHS}\frac\{\sin x(1 - \cos x)\}\{(1 + \cos x)(1 - \cos x)\} = \frac\{\sin x(1 - \cos x)\}\{1 - \cos^2 x\} = \frac\{\sin x(1 - \cos x)\}\{\sin^2 x\} = \frac\{1 - \cos x\}\{\sin x\} = \mathrm\{RHS\}

Worked Example: Proof Using Identities

Problem: Prove that 1−cos⁡2xsin⁡2x=tan⁡x\frac{1 - \cos 2x}{\sin 2x} = \tan x.

Proof:

Using cos⁡2x=1−2sin⁡2x\cos 2x = 1 - 2\sin^2 x and sin⁡2x=2sin⁡xcos⁡x\sin 2x = 2\sin x\cos x:

{1−(1−2sin⁡2x)}{2sin⁡xcos⁡x}={2sin⁡2x}{2sin⁡xcos⁡x}={sin⁡x}{cos⁡x}=tan⁡x={RHS}\frac\{1 - (1 - 2\sin^2 x)\}\{2\sin x\cos x\} = \frac\{2\sin^2 x\}\{2\sin x\cos x\} = \frac\{\sin x\}\{\cos x\} = \tan x = \mathrm\{RHS\}

Worked Example: Proof with Compound Angles

Problem: Prove that sin⁡(A+B)cos⁡Acos⁡B=tan⁡A+tan⁡B\frac{\sin(A + B)}{\cos A \cos B} = \tan A + \tan B.

Proof:

Expand sin⁡(A+B)\sin(A + B) and split the fraction:

{sin⁡Acos⁡B+cos⁡Asin⁡B}{cos⁡Acos⁡B}={sin⁡A}{cos⁡A}+{sin⁡B}{cos⁡B}=tan⁡A+tan⁡B={RHS}\frac\{\sin A \cos B + \cos A \sin B\}\{\cos A \cos B\} = \frac\{\sin A\}\{\cos A\} + \frac\{\sin B\}\{\cos B\} = \tan A + \tan B = \mathrm\{RHS\}

Common Pitfalls

Forgetting to Check All Solutions

When solving sin⁡θ=k\sin\theta = k or cos⁡θ=k\cos\theta = k There are always (at least) two solutions per Period. A common mistake is to find arcsin⁡(k)\arcsin(k) but forget π−arcsin⁡(k)\pi - \arcsin(k).

Mixing Up Degrees and Radians

Ensure your calculator is in the correct mode. If an angle is given as π3\frac{\pi}{3} It is in Radians; if given as 60∘60^\circ It is in degrees. Forgetting to convert is one of the most frequent Errors.

Wrong Sign in Compound Angle Formulas

For cos⁡(A−B)\cos(A - B):

cos⁡(A−B)=cos⁡Acos⁡B+sin⁡Asin⁡B\cos(A - B) = \cos A \cos B + \sin A \sin B

The sin⁡Asin⁡B\sin A \sin B term is positive (the ∓\mp from the ±\pm formula flips). Students often Incorrectly write a minus sign here.

Ambiguous Case of the Sine Rule

When using the sine rule with SSA data, always check whether two triangles are possible. If sin⁡B=k\sin B = k with 0<k<10 \lt k \lt 1 and BB is acute, then 180∘−B180^{\circ} - B may also be valid.

Domain of Inverse Functions

arcsin⁡x\arcsin x and arctan⁡x\arctan x return values in [−π2,π2][-\frac{\pi}{2}, \frac{\pi}{2}] While arccos⁡x\arccos x Returns values in [0,π][0, \pi]. If the actual angle is in a different quadrant, you must adjust using ASTC.

Problem Set

Problem 1: Radian Measure

Problem: A circle has radius r=8r = 8 cm. A sector of the circle has area 4848 cm2^2. Find the Exact arc length of the sector.

Solution:

Using the sector area formula A=12r2θA = \frac{1}{2}r^2\theta:

48={1}{2}(64)θ  ⟹  48=32θ  ⟹  θ={3}{2}{rad}48 = \frac\{1\}\{2\}(64)\theta \implies 48 = 32\theta \implies \theta = \frac\{3\}\{2\} \mathrm\{ rad\}

Arc length s=rθ=8×32=12s = r\theta = 8 \times \frac{3}{2} = 12 cm.

Problem 2: Compound Angle Identity

Problem: Given that sin⁡α=35\sin\alpha = \frac{3}{5} and cos⁡β=1213\cos\beta = \frac{12}{13} Where α\alpha And β\beta are acute angles, find the exact value of sin⁡(α+β)\sin(\alpha + \beta).

Solution:

Since α\alpha is acute: cos⁡α=1−925=45\cos\alpha = \sqrt{1 - \frac{9}{25}} = \frac{4}{5}. Since β\beta is Acute: sin⁡β=1−144169=513\sin\beta = \sqrt{1 - \frac{144}{169}} = \frac{5}{13}.

sin⁡(α+β)=sin⁡αcos⁡β+cos⁡αsin⁡β={3}{5}⋅{12}{13}+{4}{5}⋅{5}{13}={36}{65}+{20}{65}={56}{65}\sin(\alpha + \beta) = \sin\alpha\cos\beta + \cos\alpha\sin\beta = \frac\{3\}\{5\} \cdot \frac\{12\}\{13\} + \frac\{4\}\{5\} \cdot \frac\{5\}\{13\} = \frac\{36\}\{65\} + \frac\{20\}\{65\} = \frac\{56\}\{65\}
Problem 3: Trigonometric Equation (Factoring)

Problem: Solve 2sin⁡2x−sin⁡x−1=02\sin^2 x - \sin x - 1 = 0 for x∈[0,2π]x \in [0, 2\pi].

Solution:

Let u=sin⁡xu = \sin x: 2u2−u−1=0  ⟹  (2u+1)(u−1)=0  ⟹  u=−122u^2 - u - 1 = 0 \implies (2u + 1)(u - 1) = 0 \implies u = -\frac{1}{2} or u=1u = 1.

  • sin⁡x=−12  ⟹  x=7π6,11π6\sin x = -\frac{1}{2} \implies x = \frac{7\pi}{6}, \frac{11\pi}{6} (quadrants III and IV)
  • sin⁡x=1  ⟹  x=π2\sin x = 1 \implies x = \frac{\pi}{2}

So x=π2,7π6,11π6x = \frac{\pi}{2}, \frac{7\pi}{6}, \frac{11\pi}{6}.

Problem 4: Double Angle Application

Problem: Solve cos⁡2x=cos⁡x\cos 2x = \cos x for x∈[0,2π]x \in [0, 2\pi].

Solution:

Using cos⁡2x=2cos⁡2x−1\cos 2x = 2\cos^2 x - 1: 2cos⁡2x−1=cos⁡x  ⟹  2cos⁡2x−cos⁡x−1=02\cos^2 x - 1 = \cos x \implies 2\cos^2 x - \cos x - 1 = 0.

Let u=cos⁡xu = \cos x: (2u+1)(u−1)=0  ⟹  u=−12(2u + 1)(u - 1) = 0 \implies u = -\frac{1}{2} or u=1u = 1.

  • cos⁡x=−12  ⟹  x=2π3,4π3\cos x = -\frac{1}{2} \implies x = \frac{2\pi}{3}, \frac{4\pi}{3}
  • cos⁡x=1  ⟹  x=0,2π\cos x = 1 \implies x = 0, 2\pi

So x=0,2π3,4π3,2πx = 0, \frac{2\pi}{3}, \frac{4\pi}{3}, 2\pi.

Problem 5: Non-Right-Angled Triangle

Problem: In triangle PQR$$p = 13$$q = 14$$r = 15. Find the largest angle of the Triangle.

Solution:

The largest angle is opposite the longest side, so it is angle RR (opposite r=15r = 15).

Using the cosine rule:

cos⁡R={132+142−152}{2×13×14}={169+196−225}{364}={140}{364}={5}{13}\cos R = \frac\{13^2 + 14^2 - 15^2\}\{2 \times 13 \times 14\} = \frac\{169 + 196 - 225\}\{364\} = \frac\{140\}\{364\} = \frac\{5\}\{13\}R=arccos⁡{5}{13}≈67.4{∘}R = \arccos\frac\{5\}\{13\} \approx 67.4^\{\circ\}
Problem 6: Trigonometric Proof

Problem: Prove that tan⁡2x−sin⁡2x=tan⁡2xsin⁡2x\tan^2 x - \sin^2 x = \tan^2 x \sin^2 x.

Proof:

Starting from the LHS:

tan⁡2x−sin⁡2x={sin⁡2x}{cos⁡2x}−sin⁡2x=sin⁡2x({1}{cos⁡2x}−1)=sin⁡2x⋅{1−cos⁡2x}{cos⁡2x}=sin⁡2x⋅{sin⁡2x}{cos⁡2x}=tan⁡2xsin⁡2x={RHS}\tan^2 x - \sin^2 x = \frac\{\sin^2 x\}\{\cos^2 x\} - \sin^2 x = \sin^2 x\left(\frac\{1\}\{\cos^2 x\} - 1\right) = \sin^2 x \cdot \frac\{1 - \cos^2 x\}\{\cos^2 x\} = \sin^2 x \cdot \frac\{\sin^2 x\}\{\cos^2 x\} = \tan^2 x \sin^2 x = \mathrm\{RHS\}
Problem 7: Harmonic Form

Problem: Express sin⁡x+3cos⁡x\sin x + \sqrt{3}\cos x in the form Rsin⁡(x+α)R\sin(x + \alpha) and state the maximum Value.

Solution:

R={12+({3})2}={1+3}=2R = \sqrt\{1^2 + (\sqrt\{3\})^2\} = \sqrt\{1 + 3\} = 2tan⁡α=31=3  ⟹  α=π3\tan\alpha = \frac{\sqrt{3}}{1} = \sqrt{3} \implies \alpha = \frac{\pi}{3}

So sin⁡x+3cos⁡x=2sin⁡(x+π3)\sin x + \sqrt{3}\cos x = 2\sin\left(x + \frac{\pi}{3}\right).

The maximum value is R=2R = 2 Occurring when x+π3=π2+2nπx + \frac{\pi}{3} = \frac{\pi}{2} + 2n\pi I.e., x=π6+2nπx = \frac{\pi}{6} + 2n\pi.

Problem 8: 3D Trigonometry

Problem: A cuboid has dimensions 5×4×35 \times 4 \times 3 cm. Find the angle that the diagonal of The cuboid makes with the base.

Solution:

The space diagonal has length 52+42+32=50=52\sqrt{5^2 + 4^2 + 3^2} = \sqrt{50} = 5\sqrt{2} cm.

The projection of this diagonal onto the base has length 52+42=41\sqrt{5^2 + 4^2} = \sqrt{41} cm.

The angle θ\theta between the space diagonal and its projection onto the base is the angle with the Base:

sin⁡θ={3}{5{2}}={3{2}}{10}\sin\theta = \frac\{3\}\{5\sqrt\{2\}\} = \frac\{3\sqrt\{2\}\}\{10\}θ=arcsin⁡{3{2}}{10}≈25.1{∘}\theta = \arcsin\frac\{3\sqrt\{2\}\}\{10\} \approx 25.1^\{\circ\}

Alternatively, using the tangent:

tan⁡θ={3}{{41}}  ⟹  θ=arctan⁡{3}{{41}}≈25.1{∘}\tan\theta = \frac\{3\}\{\sqrt\{41\}\} \implies \theta = \arctan\frac\{3\}\{\sqrt\{41\}\} \approx 25.1^\{\circ\}


See Also